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1: 34.6 Definition: 9 j Symbol
§34.6 Definition: 9 j Symbol
The 9 j symbol may be defined either in terms of 3 j symbols or equivalently in terms of 6 j symbols:
34.6.1 { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } = all  m r s ( j 11 j 12 j 13 m 11 m 12 m 13 ) ( j 21 j 22 j 23 m 21 m 22 m 23 ) ( j 31 j 32 j 33 m 31 m 32 m 33 ) ( j 11 j 21 j 31 m 11 m 21 m 31 ) ( j 12 j 22 j 32 m 12 m 22 m 32 ) ( j 13 j 23 j 33 m 13 m 23 m 33 ) ,
34.6.2 { j 11 j 12 j 13 j 21 j 22 j 23 j 31 j 32 j 33 } = j ( 1 ) 2 j ( 2 j + 1 ) { j 11 j 21 j 31 j 32 j 33 j } { j 12 j 22 j 32 j 21 j j 23 } { j 13 j 23 j 33 j j 11 j 12 } .
The 9 j symbol may also be written as a finite triple sum equivalent to a terminating generalized hypergeometric series of three variables with unit arguments. …
2: 34.2 Definition: 3 j Symbol
§34.2 Definition: 3 j Symbol
The quantities j 1 , j 2 , j 3 in the 3 j symbol are called angular momenta. …They therefore satisfy the triangle conditions …The corresponding projective quantum numbers m 1 , m 2 , m 3 are given by … When both conditions are satisfied the 3 j symbol can be expressed as the finite sum …
3: 34.4 Definition: 6 j Symbol
§34.4 Definition: 6 j Symbol
The 6 j symbol is defined by the following double sum of products of 3 j symbols: …where the summation is taken over all admissible values of the m ’s and m ’s for each of the four 3 j symbols; compare (34.2.2) and (34.2.3). … The 6 j symbol can be expressed as the finite sum … where F 3 4 is defined as in §16.2. …
4: 34.11 Higher-Order 3 n j Symbols
§34.11 Higher-Order 3 n j Symbols
For information on 12 j , 15 j ,…, symbols, see Varshalovich et al. (1988, §10.12) and Yutsis et al. (1962, pp. 62–65 and 122–153).
5: 34.12 Physical Applications
§34.12 Physical Applications
The angular momentum coupling coefficients ( 3 j , 6 j , and 9 j symbols) are essential in the fields of nuclear, atomic, and molecular physics. … 3 j , 6 j , and 9 j symbols are also found in multipole expansions of solutions of the Laplace and Helmholtz equations; see Carlson and Rushbrooke (1950) and Judd (1976).
6: 34.10 Zeros
§34.10 Zeros
In a 3 j symbol, if the three angular momenta j 1 , j 2 , j 3 do not satisfy the triangle conditions (34.2.1), or if the projective quantum numbers do not satisfy (34.2.3), then the 3 j symbol is zero. Similarly the 6 j symbol (34.4.1) vanishes when the triangle conditions are not satisfied by any of the four 3 j symbols in the summation. …However, the 3 j and 6 j symbols may vanish for certain combinations of the angular momenta and projective quantum numbers even when the triangle conditions are fulfilled. Such zeros are called nontrivial zeros. …
7: 34.14 Tables
§34.14 Tables
Some selected 9 j symbols are also given. Other tabulations for 3 j symbols are listed on pp.  11-12; for 6 j symbols on pp.  16-17; for 9 j symbols on p. …
8: 34.13 Methods of Computation
§34.13 Methods of Computation
Methods of computation for 3 j and 6 j symbols include recursion relations, see Schulten and Gordon (1975a), Luscombe and Luban (1998), and Edmonds (1974, pp. 42–45, 48–51, 97–99); summation of single-sum expressions for these symbols, see Varshalovich et al. (1988, §§8.2.6, 9.2.1) and Fang and Shriner (1992); evaluation of the generalized hypergeometric functions of unit argument that represent these symbols, see Srinivasa Rao and Venkatesh (1978) and Srinivasa Rao (1981). For 9 j symbols, methods include evaluation of the single-sum series (34.6.2), see Fang and Shriner (1992); evaluation of triple-sum series, see Varshalovich et al. (1988, §10.2.1) and Srinivasa Rao et al. (1989). …
9: 10.57 Uniform Asymptotic Expansions for Large Order
Asymptotic expansions for 𝗃 n ( ( n + 1 2 ) z ) , 𝗒 n ( ( n + 1 2 ) z ) , 𝗁 n ( 1 ) ( ( n + 1 2 ) z ) , 𝗁 n ( 2 ) ( ( n + 1 2 ) z ) , 𝗂 n ( 1 ) ( ( n + 1 2 ) z ) , and 𝗄 n ( ( n + 1 2 ) z ) as n that are uniform with respect to z can be obtained from the results given in §§10.20 and 10.41 by use of the definitions (10.47.3)–(10.47.7) and (10.47.9). … For the corresponding expansion for 𝗃 n ( ( n + 1 2 ) z ) use
10.57.1 𝗃 n ( ( n + 1 2 ) z ) = π 1 2 ( ( 2 n + 1 ) z ) 1 2 J n + 1 2 ( ( n + 1 2 ) z ) π 1 2 ( ( 2 n + 1 ) z ) 3 2 J n + 1 2 ( ( n + 1 2 ) z ) .
Similarly for the expansions of the derivatives of the other six functions.
10: 26.2 Basic Definitions
If the set consists of the integers 1 through n , a permutation σ can be thought of as a rearrangement of these integers where the integer in position j is σ ( j ) . … Given a finite set S with permutation σ , a cycle is an ordered equivalence class of elements of S where j is equivalent to k if there exists an = ( j , k ) such that j = σ ( k ) , where σ 1 = σ and σ is the composition of σ with σ 1 . It is ordered so that σ ( j ) follows j . … The example { 1 , 1 , 1 , 2 , 4 , 4 } has six parts, three of which equal 1. …